Exposure time control device for an electric shutter in a single reflex camera with through the lens measuring system

ABSTRACT

A control device for controlling the exposure time automatically for an electric shutter, in a single reflex camera of the so-called &#34;through the lens&#34; photometric type which determines the brightness of an object by means of the light past through the projection lens of a camera.

This is a continuation of application Ser. No. 315,211 filed Dec. 14, 1972, now U.S. Pat. No. 3,931,628 which is a continuation of application Ser. No. 131,151, filed on Apr. 5, 1971 and now abandoned.

BACKGROUND OF THE INVENTION

This invention relates to an exposure time control device for an electric shutter.

In a single reflex camera of the "through the lens" photometric type, it is impossible to determine the brightness while the shutter is in operation. Thereupon, it has been proposed that all the while the shutter is in operation the brightness value of a photoconductive element at the time just before said shutter is operated is memorized and the exposure time is controlled automatically on the strength of said memorized value.

In such a proposition, after applying a logarithmic compression by producing the output voltage proportional to the logarithmic value of the illuminance on the light receiving surface of a photoconductive element, by means of a circuit in which photographic conditions such as setting diaphragm value, film sensitivity, etc. are set up as a bias voltage, said output voltage applied with said logarithmic compression and the bias voltage are operated photographically to allow a condenser to memorize the proper exposure time, and the memorized voltage in said condenser is applied with an inverse logarithmic conversion again to effect the automatic exposure control. And accordingly, it has the advantage of that it is possible to allow a memory condenser to memorize covering all sphere of the brightness of an object in a wide range, however, said memorized voltage is applied with a logarithmic compression so that if there should be a small error therein, in the process for applying an inverse logarithmic conversion said small error is enlarged resulting in a broad error in the exposure time.

Especially in such a proposition, behind the circuit for applying the logarithmic compression there is provided the circuit for setting up photographic conditions such as diaphragm value, film sensitivity, etc. as the bias voltage, so that in respective circuit it is necessary to do the voltage compensation and temperature compensation, and yet if this is imperfect an error which is not negligible may come out in the exposure time.

Anyway, in this manner giving the voltage compensation and the temperature compensation to respective circuit results in a very complex circuit as a whole and yet the perfect compensation can not be expected.

On the other hand, in such a circuit the exposure control is effected by an electromagnet, and while the coil of said electromagnet is in operation a large current runs therethrough so that the voltage variation of power source before and after the shutter operates is remarkable. Therefore, at the photometric time when the electromagnet coil is not operated, even though the illuminance on the light receiving surface of a photoconductive element is memorized by compressing so as to be in proportion to its logarithmic value, the power source voltage undergoes a change at the shutter operating time when the electromagnet coil is operated, therefore, when the memorized voltage memorized by compressing is applied with the inverse logarithmic conversion, on account of said voltage variation of power source an exposure control error which is not negligible comes out, and this fact stands in the way to put such a proposition to practical use.

SUMMARY OF THE INVENTION

The present invention relates to an exposure time control device in a single reflex camera with "through the lens measuring system", which is characterized in that a portion for producing the output voltage proportional to the logarithmic value of the illuminance on the light receiving surface of a photoconductive element and a bias portion for converting the setting diaphragm and the film sensitivity are connected in series to each other and said series connected body is connected to the constant-current circuit formed by one and the same power source so as to do the photographic operation, and the output voltage applied with said operation and proportional to the logarithmic value of the exposure time is memorized in a memory condenser and said memorized voltage is applied with an inverse logarithmic conversion by means of a transister for the inverse logarithmic conversion in an exposure control circuit and impressed in a time constant circuit for reversing a switching circuit.

The object of the present invention is to provide an exposure time control device in a single reflex camera with "through the lens measuring system", which effects the high precision exposure time control by memorizing the output voltage applied with a logarithmic compression proportional to the logarithmic value of the exposure time in a photometric circuit based on the photometry prior to the exposure and preventing an error to intervene into the memorized voltage in the case of that a time constant circuit for reversing a switching circuit by applying an inverse logarithmic conversion is put in operation.

Another object of the present invention is to provide an exposure time control device in a single reflex camera with "through the lens measuring system", which in order to attain the aforementioned object looks for the output voltage proportional to the logarithmic value of the illuminance on the light receiving surface of a photoconductive element and the bias voltage for converting the setting diaphragm value and the film sensitivity by means of one and the same electric power source to operate them photographically so as to allow a memory condenser to memorize its output voltage proportional to the logarithmic value of the exposure time.

Further another object of the present invention is to provide an exposure time control device in a single reflex camera with "through the lens measuring system", which operates the exposure time control circuit by applying an inverse logarithmic convertion to the memorized voltage by means of said electric power source.

Furthermore another object of the present invention is to provide an exposure time control device in a single reflex camera with "through the lens measuring system", which effects the high precision exposure time control by doing the pressure compensation for said electric power source and especially preventing the power source voltage to vary in the case of that a logarithmic compression and an inverse logarithmic conversion are applied, regardless of ON or OFF of electrification of the electromagnet coil in the exposure time control circuit.

The other object of the present invention is to provide an exposure time control device in a single reflex camera with "through the lens measuring system", in which the temperature compensation is facilitated by giving a temperature change to the constant-current of the constant-current circuit and effecting simultaneously the temperature compensation for the portion for generating the output proportional to the logarithmic value of the illuminance on the light receiving surface of the photoconductive element and the bias portion by means of the constant-current circuit formed by one and the same power source.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a circuit diagram of the control circuit in the exposure time control device in a single reflex camera with "through the lens measuring system" in accordance with the present invention.

FIG. 2 is a circuit diagram of the composite photoconductive element in the embodiment shown in FIG. 1.

FIG. 3 is a diagram showing the resistance characteristic to the logarithmic value of the illuminance on the light receiving surface in said composite photoconductive element.

FIG. 4 is a partial circuit diagram of the photometric circuit including said composite photoconductive element.

FIG. 5 is a diagram showing the relation between the potential at contact a and the illuminance on the light receiving surface in the circuit shown in FIG. 4.

FIG. 6 is a diagram showing the relation between the base voltage and the collector current of the transistor for the inverse logarithmic conversion to the temperature change.

FIG. 7 is a perspective view of the exposure time control device making use of the control circuit shown in FIG. 1, in said embodiment.

FIG. 8 is a partially enlarged view of the control circuit of the exposure time control device of another embodiment in accordance of the present invention.

FIG. 9 is a side view showing the arrangement of the composite photoconductive element in said embodiment.

DESCRIPTION OF THE PREFERRED EMBODIMENT

With reference to the drawings the present invention will be described hereinafter. FIG. 1 shows an example of the control circuit, wherein to power source E and power source switch S₁ resistance R₁ and resistance R₂ are connected in series, and connection point d thereof is connected to the base of constant-current transistor Tr₁. To the collector of said transistor Tr₁ the series connection body of composite photoconductive element R_(o) and relative resistance r₅, and the series connection body of resistances R₄ and R'₄ in parallel therewith are connected, which are connected also to the collector of temperature compensation transistor Tr₂, and said resistance R₄ is connected between the base and the collector of said temperature compensation transistor Tr₂ and the emitter thereof is connected to the negative side of power source E through variable resistance R₆ for converting the film sensitivity and the set up diaphragm value, and the parallel connection body of fixed resistance R₁₃ and thermistor R₁₄.

Said composite photoconductive element R_(o) is composed of photoconductive element R_(o1) and fixed resistance R_(x) connected in series to each other, and photoconductive element R_(o2) connected in parallel therewith as shown in FIG. 2.

To change over switch S₂ switchable to one contact a which is a connection point between said composite photoconductive element R_(o) and relative resistance R₅ and the other contact b, memory condenser C₁ is connected, and to the other end of said condenser there are connected resistances R₇, R₈ for power source voltage drop bias which are respectively connected to the positive and negative sides of the power source.

Said photoconductive elements R_(o1), R_(o2) forming composite photoconductive element R_(o) have characteristics shown in FIG. 3 for the logarithmic value of the illuminance on the light receiving surface, and the logarithm of its resistance value is inversely proportionate to the logarithm of the illuminance on the light receiving surface as shown by straight lines R_(o1) and R_(o2). On the other hand, fixed resistance R_(x) is constant relative to the logarithm of illuminance on the light receiving surface as shown by straight line R_(x), so that the logarithm of the combined resistance value of composite photoconductive element R_(o) has the characteristic shown by R_(o) to the logarithm of the illuminance on the light receiving surface. And, in the case of that to composite photoconductive element R_(o) having the resistance characteristic of the illuminance on the light receiving surface as shown in FIG. 3 relative resistance R₅ is connected in series as shown in FIG. 4, and the collector current of constant-current transistor Tr₁ is a constant-current, the relation between the potential (volt) at contact a of the connection point thereof and the illuminance on the light receiving surface is as shown by straight line f in FIG. 5, and the potential at contact a is applied with a logarithmic compression to the illuminance on the light receiving surface, and for a change of one step (1 EV) of the illuminance on the light receiving surface, V_(o) (volt) and Vo (volt) undergoes a change. Therefore, by connecting variable resistance R₆ for converting the setting diaphragm and the film sensitivity in series to relative resistance R₅ and changing said variable resistance R₆, it is possible to move the potential at contact a in parallel like straight lines shown by f₁ , f₂.

Therefore, when change over switch S₂ is connected to contact a to put a photometry into practice and the illuminance on the light receiving surface is applied with a logarithmic compression by composite photoconductive element R_(o) and relative resistance R₅ to be memorized in condenser C₁, before the shutter is operated and before the illuminance on the light receiving surface of composite photoconductive element R_(o) is not yet changed said change over switch S₂ is changed over from contact a to contact b.

Transistor Tr₃ the base of which is connected to contact b is a transistor for applying an inverse logarithmic conversion to the memorized voltage memorized in condenser C₁ by the logarithmic compression, and to condenser C₂ connected to the collector of said transistor Tr₃ the constant current proportional to the illuminance on the light receiving surface of composite photoconductive element R_(o) can be charged by opening trigger switch S₄ provided in parallel with said condenser C₂.

Main switch S₃ is closed after change over switch S₂ is disconnected from contact a, and excites electromagnet coil M. Trigger switch 4 is shut off simultaneously with the opening operation of the shutter.

Transistors Tr₄, Tr₅, Tr₆ forms a switching circuit composed of a Schmidt circuit, and when main switch S₃ is closed transistors Tr₅, Tr₆ are electrified to excite electromagnet coil M and lock the shutter from closing.

Just as trigger switch S₄ is shut off simultaneously with opening of the shutter, the voltage in memory condenser C₁, which is the result of, as described above, the voltage applied by the logarithmic compression to the illuminance on the light receiving surface of composite photoconductive element R_(o) and the voltage for converting the set up diaphragm value and the film sensitivity photographically operated, is applied with an inverse logarithmic conversion, and the constant current corresponding to the setting diaphragm value and the illuminance on the light receiving surface, and proportional to the illuminance on the light receiving surface at the time just before the shutter is operated is charged to condenser C₂, so that it is possible to control the proper exposure time in accordance with the brightness of an object, the setting diaphragm value, and the film sensitivity.

A denotes an ammeter which indicates the proper exposure time answered in accordance with the setting diaphragm value, the film sensitivity and the brightness of an object by amplifying the potential at contact a at the photometric moment by means of transistors Tr₇, Tr₈. Diode D₁ connected between the collector of said transistor Tr₇ and the base of said transistor Tr₈ is a diode for compensating the temperature.

In the present invention formed as described above, in order to effect the temperature compensation to transistor Tr₃ for the inverse logarithmic conversion, resistance R'₄ is connected between the collector and the base of temperature compensation transistor Tr₂ having the same characteristic as that of transistor Tr₃ for the inverse logarithmic conversion, and the other end of fixed resistance R₅ connected in series to photoconductive element R_(o) is connected to the collector of temperature compensation transistor Tr₂, and by using the voltage at the connection point on the collector side of said transistor Tr₂ as a bias of output terminal a and making use of the fact that the difference between the voltage of output terminal a corresponding to the resistance value of photoconductive element R_(o) and the base voltage of temperature compensation transistor Tr₂ is proportional to collector current Ic2 of said transistor Tr₂, the temperature coefficient of the bias voltage of output terminal a and the temperature coefficient of the collector current of said transistor Tr₂ are adapted to correspond to the temperature coefficient of transistor Tr₃ for the inverse logarithmic conversion so as to effect the temperature compensation to transistor Tr₃ for the inverse logarithmic conversion covering a wide extent of collector current I_(c3), and thereby an error which is not negligible in the inverse logarithmic conversion process is removed and the high precision automatic control for the exposure time can be effected covering all sphere of the illuminance on an object in a wide range.

The aforementioned fact will be described in the concrete hereinafter using formulas.

The relation between the base voltage V_(BE3) of transistor Tr₃ for the inverse logarithmic conversion and the collector current I_(c3) is expressed in general as follows:

    V.sub.BE3 = V.sub.o log.sub.2 I.sub.c3 + V.sub.1           (1)

this formula shows that when the base voltage V_(BE3) undergoes a change by V_(o), the collector current I_(c3) doubles and for a change of one step (namely, 1EV) of the exposure time, when the memorized voltage of memory condenser C₁ is changed V_(o) by V_(o) to the line form an inverse logarithmic conversion can be applied, and as described above composite photoconductive element R_(o) and fixed resistance R₅ are connected in series to each other so that the output voltage of terminal a of the connection point may be changed V_(o) by V_(o) for one step change of the illuminance on the light receiving surface.

V_(o), V₁ in formula (1) are a coefficient of transistor Tr₃ and change in accordance with the temperature respectively, and for the temperature rise V_(o) changes positively and V₁ changes negatively.

By this reason, with the progress of the temperature rise the relation between the base voltage V_(BE3) and the collector current I_(c3) undergoes a change from the solid line to the dotted line in the diagram of FIG. 6.

On the contrary, in order to compensate the temperature change of the transistor hitherto a diode has been proposed to put to use, however, the temperature compensation effected by the diode is able to be moved in parallel like the chain line shown in the diagram of FIG. 6 but it is impossible to compensate its grade, that is, as to formula (1) it is possible to compensate the temperature change of V₁ but it is impossible to compensate the temperature change of V_(o). Therefore, to carry out the temperature compensation for transistor Tr₃ for the inverse logarithmic conversion by means of a diode can not compensate covering a wide change extent of the collector current, and a considerable error comes out, and accordingly it is impossible to put to practical use in the respect of precision.

In formula (1), provided changes of V_(o), V₁ to temperature change Δt are respectively ΔV_(o), ΔV₁, change ΔV_(BE3) of the base voltage with a view in order not to change the collector current I_(c3) is as follows:

    ΔV.sub.BE3 = ΔV.sub.o log.sub.2 I.sub.c3 + ΔV.sub.1 (2)

therefore, when the output voltage of terminal a undergoes a change by ΔV_(BE3) to satisfy formula (2) to temperature change Δt, even if the temperature undergoes a change by Δt the collector current I_(c3) of transistor Tr₃ does not undergo a change, so that an error which is not negligible in the inverse logarithmic conversion process for the temperature change is compensated.

As described above, transistor Tr₂ for the temperature compensation is given the same characteristic as that of transistor Tr₃ for the inverse logarithmic conversion, so that provided the collector current of transistor Tr₂ for the temperature compensation is I_(c2), the base current V_(BE2) of transistor Tr₂ is as follows:

    V.sub.BE2 = V.sub.o log.sub.2 I.sub.c2 + V.sub.1

and, provided the difference between the base voltage of transistor Tr₂ for the temperature compensation and the output voltage of contact a is V_(a) ', and bias resistance R₄ ' connected between the collector and the base of transistor Tr₂ for the temperature compensation in FIG. 1 is not so large and the collector voltage is within the limit not saturated, V_(a) ' =αIC₂ is attained and V_(a) ' is proportional to the collector current I_(c2), and in the aforementioned formula α is a proportional constant including R₄ ', R₄, R_(o), R₅ and expressed as follows:

That is, in I_(c2), provided the current running to the R₄ side is i₁ and the current running to the R_(o) side is i₂,

    (R.sub.4 +  R.sub.4 ' ) i.sub.1 = (R.sub.o +  R.sub.5) i.sub.2, I.sub.c2 = i.sub.1 +  i.sub.2 (R.sub.4 +  R.sub.4 ' )(I.sub.c2 -  i.sub.2 ) = (R.sub.o +  R.sub.5 ) i.sub.2

Therefore, ##EQU1## And, making use of

    V.sub.a ' = -  R.sub.4 '  i.sub.1 +  R.sub.5 i.sub.2 =  R.sub.4 '  i.sub.2 +  R.sub.5 i.sub.2 -  R.sub.4 '  I.sub.c2

as the results, ##EQU2## Therefore, ##EQU3## Therefore, the output voltage V_(a) of contact a is as follows:

    V.sub.a =  R.sub.6 I.sub.c2 +  V.sub.BE2 + V.sub.a ' = R.sub.6  I.sub.c2 + V.sub.o log.sub.2  I.sub.c2 + V.sub.1 +α I.sub.c2

Change ΔV_(a) of the output voltage of contact a to the temperature change Δt is as follows:

    ΔV.sub.a =  R.sub.6 Δ I.sub.c2 + Δ V.sub.o log.sub.2 I.sub.c2 + V.sub.o (ΔI.sub.c2 /I.sub.c2 log.sub.e 2) + ΔV.sub.1 + αΔ I.sub.c2

Whereas, V_(o) (1 /I_(C2) log 2) is small as compared with other coefficients and negligible, and it is possible to effect this temperature compensation by means of thermister R₁₄ connected to variable resistance V₆ and fixed resistance R₁₃, so that

    ΔV.sub.a = R.sub.6 Δ I.sub.c2 + Δ V.sub.o log.sub.2 I.sub.c2 + Δ V.sub.1 + αΔ I.sub.c2

As described above, when in ΔV_(a) = Δ V_(BE3) , even if the temperature undergoes a change by Δt the collector current I_(c3) of transistor Tr₃ for the inverse logarithmic conversion does not undergo a change, so that the temperature compensation for the inverse logarithmic conversion process is enough effected and the exact automatic exposure time can be obtained.

Change Δ I_(c2) of the collector current of transistor Tr₂ for the temperature compensation in order to be ΔV_(a) = Δ V_(BE3) is given the following relation:

    R.sub.6 Δ I.sub.C2 + Δ V.sub.o log.sub.2 I.sub.c2 + Δ V.sub.1 + αΔ I.sub.c2 = Δ V.sub.o log.sub.2 i + Δ V.sub.1 (R.sub.6 + α) ΔI.sub.c2 = Δ V.sub.o log.sub.2 (I.sub.c3 /I.sub.c2 )                                     (3)

As shown in the aforementioned formula, the temperature change ΔV₁ of coefficient V₁ of transistor Tr.sub. 3 for the inverse logarithmic conversion is compensated by the temperature change (ΔV_(o) log I_(c2) + ΔV₁ ) of the bias of the output terminal.

And, V_(BE3) = V_(a), therefore, ##EQU4## From formula (3) ##EQU5##

Therefore, when the temperature change of the collector current I_(c2) of transistor Tr₂ for the temperature compensation satisfies formula (4). not only the temperature change of coefficient V₁ of transistor Tr₃ for the inverse logarithmic conversion but also the temperature change of V_(o) is compensated. The temperature change of the collector current I_(c2) of transistor Tr₂ for the temperature compensation is carried out making use of the temperature change of the base voltage V_(BE1) of constant-current transistor Tr₁.

Provided the voltage of point d divided by resistances R₁, R₂ is V_(d), the current for running to resistance R₃ runs almost all to the collector of transistor Tr₁ and this current becomes the collector current I_(c2) of transistor Tr₂, therefore, R₃ I_(c2) + V_(BE1) =V_(d),

Whereas, V_(d) does not undergo a temperature change, so that when the temperature undergoes a change by Δt change ΔI_(c2) of the collector current I_(c2) is as follows: ##EQU6## Therefore, from formula (4) ##EQU7##

When the temperature undergoes a change by Δt, by fixing resistances R₁, R₂ so that the temperature ΔV_(o) of coefficient V_(o) of transistor Tr₃ for the inverse logarithmic conversion may get to be V_(d) for satisfying formula (5), the temperature compensation of coefficients V_(o), V₁ of transistor Tr₃ for the inverse logarithmic conversion can be effected, and the high precision automatic exposure time control can be carried out.

Variable resistance R₆ is a resistance for converting the setting diaphragm value and the film sensitivity as described above, and by increasing or decreasing both ends voltage R₆ I_(c2) of said variable resistance R₆ V_(o) by V_(o) into the line form the setting diaphragm value or the film sensitivity can be changed by one step, and at the same time, when the collector current of temperature compensation transistor Tr₂ undergoes a temperature change for satisfying formula (4), formula (4) does not include R_(o), R₆ so that the temperature change of transistor Tr₃ for the inverse logarithmic conversion can be compensated continuously to an optional value of R₆, R_(o), therefore, the both ends bias voltage of variable resistance R₆ for converting the setting diaphragm value and the film sensitivity effects the temperature compensation of transistor Tr₃ for the inverse logarithmic conversion to the brightness of an object, and the conversion of the setting diaphragm value and the film sensitivity can be carried out.

As described hereinbefore, in the present invention the portion for producing the output voltage proportional to the logarithmic value of the illuminance on the light receiving surface of the photoconductive element and the portion for converting the setting diaphragm value and the film sensitivity are connected in series to each other and connected to one and the same power source, and at the same time the photographical operation is effected to them and through the collector current I_(c2) of temperature compensation transistor Tr₂ the temperature compensation is effected to the optional brightness, the setting diaphragm, and the film sensitivity so that it is possible to effect the temperature compensation at the same time and the high precision automatic control for the exposure time can be effected covering all sphere of the brightness of an object in a wide range.

Next, when electromagnet coil M is excited a large current runs thereto, so that the voltage undergoes broadly a change as well known, therefore, when electromagnet coil M operates before the shutter is operated the power source voltage undergoes a change and accordingly an error of the exposure time comes out on account of variation of the trigger level of the Schmidt circuit. However, in the present invention, in order to compensate said error resistances R₇, R₈ for giving the bias voltage to memory condenser C₁ are provided.

Provided the amplification rate of transistor Tr₅ is β, trigger voltage V_(T) of the Schmidt trigger circuit is as follows:

    V.sub.T =  (β R.sub.9 /β R.sub.9 +  R.sub.10) V =  B.sup.. V (6)

(v is the power source voltage)

After switch S₂ shuts off terminal a and memorizes, just as main switch S₃ is electrified electromagnet coil M is exited and a large current runs, so that power source voltage V undergoes broadly a change to drop and trigger voltage V_(T) drops in proportion to power source voltage V, and thereby an error is made. In order to compensate this error resistances R₇, R₈ are provided to give the bias to memory condenser C₁.

Provided the memory voltage of condenser C₁ is V_(c), the power source voltage is V, and the voltage of bias resistance R₈ proportional to V is XV,

    v.sub.be3 = v.sub.o log.sub.2 I.sub.c3 +  V.sub.1 =  V.sub.c +  XV (7)

and, provided the capacity of condenser C₂ is C₂ and the time required for condenser C₂ to gets to the trigger voltage is T,

    c.sub.2 v.sub. t = i.sub. c3 T                             (8)

and thus, change of V_(T) to change of power source voltage V is as follows from formula (6): ##EQU8##

Electromagnet coil M operates and the power source voltage undergoes a change by ΔV, and accordingly when trigger voltage V_(T) undergoes a change by ΔV_(T), change of I_(c3) for fixing the exposure time T is as follows from formula (8): ##EQU9## and from formula (7) ##EQU10##

Therefore, bias voltage XV of memory condenser C₁ for which change of the collector current of transistor Tr₃ at the time when the power source voltage undergoes a change by ΔV satisfies formula (9) is as follows: ##EQU11##

Therefore, making use of formulas (6), (8), ##EQU12##

Therefore, after applying the bias for satisfying formula (11) to memory condenser C₁ and switch S₂ shuts off terminal a to memorize, just as main switch S₃ is electrified the variation of the trigger level in the Schmidt circuit caused by a broad variation of power source voltage V due to the exitation of electromagnet coil M is compensated by change of collector current I_(c3) caused by change of the base voltage V_(BE3) of transistor Tr₃ due to the bias for satisfying formula (11), and the exact exposure time can be obtained.

FIG. 7 is a perspective view showing the shutter mechanism in a "through the lens" photometric type focal plane single reflex camera in the case of that the exposure time control circuit shown in FIG. 1 is applied to said camera, and the essential portions of an embodiment in the mechanical interlocking relation with the electromagnet, resistors, switches, etc. in the circuit in accordance with the present invention.

Interlocking wire 4 fixed on its one end to pulley 3 connected by axle 2 to film sensitivity setting dial 1 provided on the camera body so as to rotate in a body with said dial 1 is fixed on its other end to diaphragm setting ring 7 of the lens barrel via pulley 6 pivoted on arm portion 5a projecting in the radial direction from gear 5 fitting loosely on said axle 2. And, slide brush 9 provided on insulating axle 8a for gear 8 meshed with said gear 5 is adapted to slide on variable resistance R₆.

Therefore, just as the film sensitivity is set up by means of film sensitivity setting dial 1 and the diaphragm value is set up by means of diaphragm setting ring 7, said slide brush 9 slides on variable resistance R₆ so as to get the value corresponding to the setting film sensitivity and the setting diaphragm value. Said brush 10 is a stationary brush.

When the camera is put to use electric power source switch S₁ not shown in FIG. 7 is put in the conductive state. Therefore, the circuit shown in FIG. 1 is in the photometric state and ammeter A not shown in the drawing is in indicating the exposure time.

Photoconductive element R_(o) is provided on pentagonal prism 11 and its composite photoconductive element R_(o) effects the photometry actually.

Now, just as shutter button 12 is pushed interlocking lever 13 is pushed down and lever 15 is turned counterclockwise by interlocking rod 14 to disengage from switch lever 16 having the turning tendency to the direction shown by arrow CW₃. Thereupon, pin 17a for insulating member 17 for changing over the switch fixed to said switch lever 16 changes over switch S₂ from contact a to contact b and after switch S₂ shuts off contact a pin 17b for insulating member 17 closes main switch S₃ to exite electromagnet coil M.

After main switch S₃ is electrified, switch lever 16 turns mirror lever 19 to the direction shown by arrow CW₄ through intermediate lever 18 and also turns reflector 21 to the same direction through axle 20. Therefore, through the turning of said reflector 21 the photometric state is changed to the photographing state and the quantity of light incoming to photoconductive element R_(o) is decreased gradually, however, switch S₂ is already changed over from contact a to contact b so that the resistance value of composite photoconductive element R_(o) under the photometric state is memorized.

In the final process, mirror lever 19 engages with release lever 22 to turn it and the pawl of opening screen restraining lever 23 disengage from restraining plate 24, and restraining plate 24 turns together with the opening screen axle having the turning tendency to the direction shown by arrow CW₂ via axle 25, and gears 26, 27 and opening screen 32 starts to open the shutter. And at the same time, protrusion 28 fixed to axle 25 turns counterclockwise to open trigger switch S₄ for condenser C₂ so that said condenser C₂ is charged.

However, the closing screen is in being checked against travelling by closing screen restraining lever 29 attracted by electromagnet coil M. Just as the voltage of condenser C₂ gets to the trigger voltage V_(T), electromagnet coil M is demagnetized and closing screen restraining lever 29 turns clockwise through spring 30 so as not to engage lever 29 with pin 31a and gear 31 becomes turnable so that shutter closing screen 34 starts to travel via gear 33 to close the shutter.

Just as winding lever 35 is turned counterclockwise the film not shown in the drawing is wound and at the same time gear 26 is turned clockwise via gears 36, 37, 38, 39 formed in a body with said winding lever 35, and when restraining plate 24 formed in a body with gear 26 engages with the pawl of opening screen restraining lever 23 the shutter charge is finished.

Since the present invention is formed as described hereinbefore, the memory condenser is in memorizing the voltage proportional to the logarithmic value of the exposure time so that it is possible to memorize the voltage covering all sphere of the brightness of an object in a wide range, and in addition as described above it is easy to operate the output voltage proportional to the logarithmic value of the illuminance on the light receiving surface of the composite photoconductive element and the voltage for converting the setting diaphragm value and the film sensitivity, and it is possible to effect the temperature compensation at the same time to these lightness, setting diaphragm value, and film sensitivity and that by carrying out the temperature compensation of transistor Tr₃ for the inverse logarithmic conversion covering a wide extent of the collector current IC₃ of said transistor Tr₃ it is possible to remove an error which is not negligible in the inverse logarithmic conversion process, and besides an error of the exposure time control caused by a broad variation of the power source voltage due to the exitation of electromagnet coil M can be compensated as well.

FIG. 8 is a partial circuit diagram of another embodiment in accordance with the present invention, wherein the respect differing from the embodiment shown in FIG. 1 is that composite photoconductive elements R_(o), R_(o) ' are directly connected. Said composite photoconductive elements R_(o), R_(o) ' are respectively provided in the separate position on pentagonal prism 11 as shown in FIG. 9. The light rays past through the objective lens are reflected by reflector 21 and come to focusing screen 40, and are diffused hereby and through condenser lens 41, pentagonal prism 11, and eye piece 42 the focussing image can be observed. And at the same time, a portion of the diffusion light rays come to composite photoconductive elements R_(o), R_(o) ' and the light rays past through the objective lens are measured, however, composite photoconductive elements R_(o), R_(o) ' disposed as shown in FIG. 9 are in measuring different portions of an object in dividing respectively.

Provided that the resistance-illuminance characteristics of two simple substance photoconductive elements are both identical and R=KL⁻.sup.β, in the case of the divisional photometry described above when the light rays in the illuminances of L₁ and ML₁ come into two photoconductive elements respectively the whole resistance value R (L₁, ML₁) of said two photoconductive elements connected in series is as follows: ##EQU13##

And, when light rays of M'L₁ come into in the illuminance equivalent to two photoconductive elements the resistance value R(M'L₁, M'L₁) of the series connected body is as follows: ##EQU14##

And, when this is satisfied,

    R(L.sub.1, ML.sub.1) = R (M'L.sub.1, M'L.sub.1)

in this manner, it is well known that by connecting photoconductive elements for doing divisional photometry in series and averaging objects different in the brightness ratio so as to satisfy formula (12), the photometry of good probability can be effected which turns to the proper exposure. In this case, especially when in γ = 0.62 it has been reported that the probability to turn to the proper exposure is the largest.

Then, as to the series connected body of composite photoconductive elements R_(o), R_(o) ' as shown in FIG. 8, the illuminance-resistance characteristics of elements R_(o1), R_(o2) for constituting composite photoconductive element R_(o) and elements R_(o3), R_(o4) for constituting composite photoconductive element R_(o) ', as seen in FIG. 3, satisfy the following formulas: ##EQU15##

When light rays in the illuminances of L₁, ML₁ come into said composite photoconductive elements R_(o), R_(o) ' respectively the resistance values R'(L₁, ML₁) of the series connected body is as follows: ##EQU16##

And, when light rays of M'L₁ come into in the illuminance equivalent to two composite photoconductive elements R_(o), R_(o) ' the resistance value R'(M'L₁, M'L₁) of said series connected body is as follows: ##EQU17##

When this is satisfied it turns to R'(L₁, ML₁) = R'(M'L₁, M'L₁).

And accordingly, the resistance value of the series connected body in the case of that light rays in the illuminances of L₁, ML₁ come into two composite photoconductive elements for doing divisional photometry as shown in FIG. 8 respectively turns to the resistance value in the case of that light rays in the equal illuminances of M'_(k), L₁ come into composite photoconductive elements R_(o), R_(o) '.

This fact shows that in the same way as the series connected body of two simple substance photoconductive elements for doing divisional photometry, the series connected body of two composite photoconductive elements for doing divisional photometry as shown in FIG. 8 is in averaging objects different in the brightness ratio so as to satisfy the same formula (12). Therefore, the series connected body of composite photoconductive elements shown in FIG. 8 becomes possible to do photometry of the good probability which turns to the proper exposure to objects different in the brightness ratio, in the same manner as in the series connected body of simple substance photoconductive elements for doing divisional photometry. Especially in the case of that γ of elements R_(o1), R_(o2), R_(o3), R_(o4) constituting composite photoconductive elements R_(o), R'_(o) is γ = 0.6, the photometry which probability to turn to the proper exposure is the best becomes possible. 

We claim:
 1. In an electric shutter control device for a single lens reflex camera having a light receptive element for receiving light through an objective lens of the camera, a light detecting circuit having said light receptive elements for generating an output voltage proportional to the logarithm of the light intensity incident on said light receptive element, means for storing said output voltage during operation of the shutter, a first transistor for detecting the voltage stored by said means for storing and for generating a current output, said current output being proportional to the antilogarithm of said stored voltage, means for integrating said current output, and means responsive to said integrated current for initiating closing of the shutter after a time interval determined by said integrated current, the improvement whereinsaid light detecting circuit further has an output resistance serially connected with said light receptive element and a resistance shunting said serially connected light receptive element and said output resistor, said output voltage being generated at the junction point of said output resistance and said light receptive element, and a second transistor having substantially the same electric and temperature characteristics as said first transistor and further having a collector connected to one terminal of the parallel combination of said shunting resistance and said serially connected light receptive element and said output resistance, and a base connected to said shunting resistance to be biased thereby, and a third transistor for supplying constant current to the collector of said second transistor whereby said second transistor compensates for variations in said integrated current due to changes in temperature.
 2. An exposure control device as set forth in claim 1, wherein the temperature characteristic of the collector current of said second transistor is substantially equal to the temperature characteristic of the collector current of said first transistor, whereby said output voltage is compensated in accordance with the formula ΔV₀ /V₀ = ΔI_(c2) /I_(c2), wherein V₀ is said output voltage, ΔV₀ is the change in said output voltage, ΔI_(c2) is the change in collector current of said second transistor, and I_(c2) is the collector current of said second transistor.
 3. An exposure control device as set forth in claim 2, further comprising means for generating constant current including said third transistor, a voltage divider circuit having a third and a fourth resistance for biasing said third transistor, and the respective resistances of said third and fourth resistances are such that the temperature characteristic of the collector current of said first transistor is substantially equal to the temperature change characteristic of the voltage between the base and the emitter of said third transistor in accordance with the formula ΔI_(c2) /I_(c2) = ΔV_(BE1) /V_(BE1) - V_(d), wherein V_(BE1) and ΔV_(BE1) are the base-to-emitter voltage of said third transistor and V_(d) is the voltage at the junction of said third and fourth resistances.
 4. An electric shutter control device as in claim 1 further comprising means for varying said constant current in dependence upon temperature changes in the surroundings in accordance with the following formula: Δi = ΔV₀ V₀ wherein Δi is the change in said constant current with temperature, ΔV₀ is the change of V₀ with temperature, V₀ is defined by V_(o) = V_(BE2) - V₁ /log₂ I_(c2) and wherein V_(BE2) is the base-to-emitter voltage of said second transistor, I_(c2) is the collector current of said second transistor, V₀ and V₁ are the coefficients showing the relationship between base-emitter voltage and collector current of a transistor, which coefficients change with changes in temperature.
 5. An electric shutter control device as in claim 1 further comprising biasing means including a variable resistor connected in series with the emitter of said second transistor for generating additional voltage to be added to the output voltage of said light detecting circuit, and means for adjusting said variable resistor in accordance with setting of a value of film sensitivity.
 6. An exposure control device as set forth in claim 5, further comprising diaphragm aperture setting means and wherein the resistance value of said biasing means is also varied in accordance with the setting of said diaphragm aperture setting means.
 7. An electric shutter control device as set forth in claim 5, wherein said shunting resistance includes two resistances connected together and said second transistor base is connected to the junction of said two resistances.
 8. In an electric shutter control device for a camera including light receptive means receiving scene light through an objective lens of the camera and generating a signal indicative of the light incident thereon, a light detecting circuit having said light receptive means and for generating an output voltage proportional to the logarithm of the light intensity incident on said light receptive means, means for storing said output voltage during shutter operation, means for timing the closing of the shutter in accordance with said stored voltage, said means for timing having an integrating capacitor and a first transistor coupled to said capacitor, the improvement comprising:means for setting a value of film sensitivity; means including a linearly variable resistor adjustable in accordance with the setting of said film sensitivity for generating an additinal voltage comprising part of said output voltage; and means for applying constant current to said variable resistor, and including a second transistor and a resistor connected to the emitter of said second transistor, the collector of said second transistor generating said constant current, said means for generating constant current further including means for generating an operating voltage between the base of said second transistor and the other terminal of said resistor, said constant current being changed in response to temperature changes in the surroundings in accordance with the following formula Δi/i = ΔV₀ /V₀ wherein Δ i is the change in said constant current with temperature, ΔV₀ is the change of V₀ with temperature, V₀ is defined by V₀ = V_(BE) - V₁ /log₂ I_(c) and wherein V_(BE) is the base-emitter voltage of said first transistor, I_(c) is the collector current of said first transistor, V₀ and V₁ are the coefficients showing the relationship between base-emitter voltage and collector current of said first transistor, which coefficients change with changes in temperature.
 9. In an electric shutter control device for a photographic camera, a combination comprising:a light measuring circuit including a light receptive element and means for generating an output voltage representative of light incident on said light receptive element; means for storing said output voltage during a shutter operation; means for determining duration of exposure in accordance with said output voltage and including a first transistor and an integrating capacitor connected to the output of said first transistor; a second transistor for generating a biasing potential at the collector thereof in accordance with changes in temperature, said biasing potential being included in said output voltage for preventing temperature dependent changes in the output of said first transistor; a resistor connected between the collector and the base of said second transistor; means for generating a constant current i which is variable with changes in temperature as given by the following formula, Δi/i = ΔV₀ /V₀ wherein Δ i is the change in said constant current with temperature, Δ V₀ is the change with temperature, V₀ is defined by V₀ = V_(BE) -v₁ /log₂ I_(c) and wherein V_(BE) is the base-to-emitter voltage of said first transistor, I_(c) is the collector current of said first transistor, V₀ and V₁ are the coefficients showing the relationship between base-emitter voltage and collector current of said first transistor, which coefficients change with changes in temperature; and said means for generating constant current is connected to the collector of said second transistor, whereby the effect of temperature changes to the electrical characteristics of said first transistor is compensated by said second transistor.
 10. An electric shutter control device as set forth in claim 9, further comprising variable resistor means connected between the emitter of said second transistor and the ground of said device.
 11. An electric shutter control device as set forth in claim 9, further comprising means for setting a value of film sensitivity including a variable resistor connected to the emitter of said second transistor and adjustable in accordance with the film sensitivity setting. 